Magnetic resonance apparatus and method for parallel imaging with a reference data set for determining the weighting matrix

ABSTRACT

In a magnetic resonance apparatus and a method for generating MR image data of a subject with parallel imaging, a reference data set of the object is recorded, in which at least one partial section of the associated raw data space is completely filled with raw data according to the Nyquist condition, and an imaging data set is recorded for the generation of the MR image data on the basis of spin-echo-based signals, in which the associated raw data space is not completely recorded according to the Nyquist condition. A weighting matrix is calculated based on the reference data set, which is used to determine raw data points of the imaging data set not recorded during parallel imaging. The unrecorded raw data points of the imaging data set are calculated using the calculated weighting matrix. The reference data set is recorded with a spin-echo-based reference imaging sequence without segmentation within an imaging slice and without temporal overlap with the recording of the imaging data set, and a resolution is used in the readout direction which is lower by at least a factor of 4 than when the imaging data set is recorded.

BACKGROUND OF THE INVENTION Field of the Invention

The present invention concerns a method for generating magneticresonance (MR) image data of an object under examination with parallelimaging, and an MR system and an electronically readable data storagemedium that implement such a method.

Description of the Prior Art

MR systems having a cylindrical geometry have a reduced homogeneity ofthe constant magnetic field B0 and a reduced gradient linearity at theedges of the field of view in the bore direction, which is usuallyreferred to as the z-axis. For coronary and sagittal recordings, thisleads to compressed regions in the reconstructed images with high signalintensity in the regions at the edge of the bore, since theinhomogeneity of the gradient field and/or of the polarization field B0means that a number of regions of the object under examination aremapped to a relatively small image region, which increases the signalintensity in this image region and conversely decreases the signalintensity in adjacent regions. This means that, as a result of theincorrect position encoding, both pixels with an increased signalintensity, and pixels with a reduced signal intensity, exist. Theseregions are generally located at the edge of the field of view (FOV) inthe z-direction. Moreover, the use of parallel imaging techniques, suchas GRAPPA, often results in artifacts occurring at integer multiples ofthe position FOVz/R in imaging sequences, where R is the accelerationfactor. In parallel imaging, the missing unmeasured raw data areas arecalculated with the use of a number of receive channels and theirdifferent coil sensitivities. The coil sensitivities are ascertained byreference measurements or calibration measurements. This procedurerequires a good reference data set or calibration data set. If thelatter is faulty, then the MR images calculated with parallel imagingare also faulty. The reason for the artifacts in parallel imaging isalso that the imaging algorithms are usually not able to handlelocalized regions with very high signal intensity, which, as explainedabove, can occur at the edge of the MR system components. In parallelimaging in particular, this leads to the incomplete suppression ofso-called aliasing artifacts in these regions.

This phenomenon is particularly prominent in spin echo sequences becausedephasing plays a lesser role in such sequences on B0 inhomogeneities orgradient inhomogeneities, and does not lead to signal cancelation as inthe case of gradient echo sequences. In addition, the intensity and formof the aforementioned artifacts are dependent on the recordingparameters (such as gradient amplitudes, bandwidth of the RF pulses,reception bandwidth, and image resolution).

A further factor that can lead to the recording of a faulty calibrationdata set is the segmented recording of the calibration data. This meansthat the required k-space data are not recorded consecutively in a shorttime sequence but rather are recorded in segments over a longer periodof time. This is the case when the data are obtained in the context ofrecording the imaging data. Physiological effects such as blood flow,liquor pulsation, heartbeat and respiration then lead to inconsistenciesin the data recorded in segmented fashion, for example with regard totheir phase position relative to one other.

One way of reducing these artifacts is to average the MR signals byrecording the MR signals twice or multiple times. If the MR signals arerecorded twice, this can take place once with recording (filling) of theeven k-space lines and once with recording of the odd k-space lines. Thecentral k-space lines of both recordings are then combined and used tocalculate the reference data sets or calibration data sets. Theartifacts in the final composite image are canceled out by such amethod, but the measurement time is at least doubled, which is asignificant disadvantage.

SUMMARY OF THE INVENTION

An object of the invention is to reduce the aforementioned disadvantagesin order to improve parallel imaging such that fewer artifacts arepresent in the reconstructed image data.

In a method according to the invention for generating MR image data ofan object under examination with parallel imaging, a reference data setof the object under examination is recorded, in which at least onepartial section of the associated raw data space (k-space) is completelyfilled with raw data according to the Nyquist condition. Furthermore, animaging data set for the generation of MR image data is recorded on thebasis of spin-echo based signals, in which case the associated raw dataspace is not completely recorded according to the Nyquist condition. Aweighting matrix is calculated on the basis of the reference data set,which is used to determine raw data points of the imaging data set thatwere not recorded during parallel imaging. The unrecorded raw datapoints of the imaging data set are calculated using the calculatedweighting matrix. In this case, the reference data set is recorded witha spin-echo-based reference imaging sequence without segmentation of therecording data within an imaging slice and without temporal overlap withthe recording of the imaging data set, and the resolution in the readoutdirection is lower by at least a factor of four than when the imagingdata set is recorded.

Despite its name, the aforementioned imaging data set contains raw MRdata, which are reconstructed into MR image data, and the reconstructedMR image data are displayed at a display monitor as an MR image of theexamination subject. For this purpose, the completed raw data set,formed by applying the weighting matrix to the incomplete acquired rawdata set, is made available as a data file, for storage and/or forimplementing the aforementioned reconstruction.

The resolution in the readout direction can be reduced by using atemporally separated reference data set which does not overlaptemporally with the recording of the imaging data set. This reduces therecording time for the reference data set and allows the imagingparameters for the reference data set to be selected independently ofthe parameters for creating the imaging data set. Preferably, theimaging data set is recorded in segmented fashion and entered into anumber of recording regions within a number of imaging slices, in whichcase the reference data set is recorded for each of the multiple imagingslices. If the imaging for the creation of the MR image data is amulti-slice sequence, then the reference data set for the actual slicecan be recorded before or after the recording of that slice.

For example, it is possible that the RF excitation pulse used in orderto generate the spin echo when creating the imaging data set may have adifferent slice profile than the RF excitation pulse that is used whencreating the reference data set. Similarly, the slice profile of therefocusing pulses that are used when creating the imaging data set maybe different from that of the RF refocusing pulses that are used whencreating the reference data set.

Furthermore, when creating the reference data set, RF refocusing pulsesafter a first RF refocusing pulse can be used in order to generate thespin echoes, which have a smaller flip angle than the corresponding RFrefocusing pulses that occur after the first refocusing pulse whencreating the imaging data set. The flip angles of the RF refocusingpulses after the first RF refocusing pulse can be between 20° and 120°in the case of the reference data set, preferably between 20° and 70°.As a result of the smaller flip angles, the recording time can bereduced in total because the time required for radiation by the RFpulses can be reduced. Furthermore, the radiated energy can be reducedby the smaller flip angles.

It is likewise possible when creating the reference data set to use RFexcitation pulses and refocusing pulses whose spectral bandwidth isindependent of the spectral bandwidth of the RF excitation pulses andrefocusing pulses that are used when creating the imaging data set. Forexample, it is possible to select the spectral bandwidth the same in thecase of the RF excitation pulse and the RF refocusing pulse in the caseof the reference data set. This is not the case as a general rule whencreating the imaging data set.

Furthermore, it is possible to select the RF pulses used when creatingthe reference data set such that they have an average reference durationthat is shorter by a factor of at least 0.8 than the average duration ofthe RF pulses that are used when creating the imaging data set.

By means of the aforementioned capabilities of the inventive method, itis possible to record the reference data set in a very short time. Thisreference data set also has a good brightness and a homogeneousdistribution of the signal over the entire image data space. It isthereby possible to accurately calculate the weighting matrix and thecoil sensitivities for the individual receive coils. By separating therecording of the raw data set and the imaging data set, it is possibleto create raw data sets that are better suited for the calibration ofparallel imaging, since there is no need to take into account theparameters used of the imaging data set.

For example, the imaging data set can be a turbo spin echo Dixonsequence. In such a sequence, spin echoes of different tissue componentsat least have the same phase position once and an opposite phaseposition once. In the prior art it was usual to record the referencedata set interleaved with the actual imaging data set. Particularly witha turbo spin echo Dixon sequence, this led to unsatisfactory results inthe creation of the reference data set since the spacing of therefocusing pulses needs to be increased in order to fulfill thecondition for opposing phase positions. If the reference data set isobtained from the data with the same phase position, the physiologicaleffects described above become more noticeable. However, if it isascertained from the data with the opposite phase position, therecording times are not located in the center between two pulses, whichresults in an additional dephasing of the spins in the marginal regionsof the FOV, which has a negative effect on the calibration as describedabove.

The invention furthermore concerns an associated MR apparatus forcreating the MR image data with the use of the reference data set andthe weighting matrix described above. The MR apparatus has a controlcomputer and a memory in which control information is stored that can beexecuted by the control computer in order to operate the scanner of theMR apparatus. The MR apparatus is designed to carry out the stepsdescribed above and also described in detail below when the controlinformation is executed in the control computer.

The present invention also encompasses a non-transitory,computer-readable data storage medium encoded with programminginstructions that, when the storage medium is loaded into a computer orcomputer system of a magnetic resonance apparatus, cause the computer orcomputer system to operate the MR apparatus in order to execute any orall embodiments of the method according to the invention, as describedabove.

The features described above and the features described below can beused not only in the correspondingly explicitly stated combinations butalso in other combinations, unless explicitly stated otherwise.Furthermore, the various features described can be used individually.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 schematically shows an MR apparatus with which, according to theinvention, when implementing parallel imaging, artifacts can be reducedin the image calculation by an improved weighting matrix, which iscalculated on the basis of a reference data set.

FIG. 2 schematically shows an example of an MR image in which anartifact occurs in a marginal region, which can be avoided with the MRsystem shown in FIG. 1.

FIG. 3 schematically shows a sequence for the creation of the referencedata set, with which the artifacts of FIG. 2 are reduced.

FIG. 4 shows a flowchart of an exemplary embodiment of the inventivemethod with steps for improved recording of a reference data set, whichenables an improved calculation of the weighting matrix.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIG. 1 schematically shows an MR system with which, according to theinvention, artifacts in MR images can be reduced that are caused by anunsatisfactory reference data set being used during parallel imaging inorder to calculate a weighting matrix, the so-called kernel. Themagnetic resonance system has an MR data acquisition scanner with magnet10 that generates a polarization field B0. A person under examination,on a patient bed 11, constitutes the object under examination 12, who isintroduced into an isocenter Z0 of the magnet 10 in order to recordspatially encoded magnetic resonance signals from the object underexamination 12. As is explained in more detail below, the recordingvolume usually has a first recording region with a higher inhomogeneityof fields and a second recording region in which the homogeneity of therespective fields is better than in the first subregion. Thepolarization field B0 and/or the linearity of the magnetic fieldgradients that are generated by gradient coils (not shown) for thespatial encoding can be considered here as the relevant fields. Byradiating with radio-frequency (RF) pulses and switching magnetic fieldgradients, the magnetization of certain nuclear spins in the object 12generated by the polarization field B0 is deflected from the steadystate and the signals emitted by those spins as they relax and return tothe steady state are detected as currents induced in reception coils 5to 8, as magnetic resonance signals. The general operation for thecreation of MR images utilizing the detection of magnetic resonancesignals, in particular with regard to parallel imaging using a weightingmatrix for the generation of unrecorded raw data points, is known tothose skilled in the art, so that a more detailed description is notnecessary herein.

The magnetic resonance apparatus has a control computer 13 that operatesthe MR apparatus. The control computer 13 has a gradient controller 14for controlling and switching the magnetic field gradients and an RFcontroller 15 for generating and controlling the RF pulses in order todeflect the nuclear spins from the steady state. The RF controller 15 isa multi-channel RF component, which generates RF pulses in a number ofindependent channels. A memory 16 stores the imaging sequences necessaryfor recording the MR images, as well as all other control informationnecessary to carry out the invention. An image sequence controller 17controls the image recording (data acquisition) and thus, depending onthe selected imaging sequences, the sequence of the magnetic fieldgradients, the RF pulses and the receive intervals of the MR signals. Inthis way, the image sequence controller 17 also controls the gradientcontroller 14 and the RF controller 15. MR images, which can bedisplayed on a display 18, are calculated (reconstructed) in a processor20. An operator can control the MR system via an input unit 19. Theprocessor 20 is used, inter alia, in order to calculate a weightingmatrix, or the so-called kernel, such as the GRAPPA kernel, on the basisof a reference data set.

FIG. 2 schematically illustrates an MR image 22, which shows an MR imageof a first object under examination 23 and a second object underexamination 24. The object under examination 24 is positioned at theedge of the MR system in the phase encoding direction, in other words atthe edge at which the homogeneity of the polarization field B0 is lowerand at which the linearity of the magnetic field gradients is lower thanin the region in which the object 23 is arranged. With regard to theembodiment shown in FIG. 2 it is assumed that the first object underexamination 23 is essentially centered in the isocenter Z0 of themagnet. A first homogeneity of the polarization field B0 and of themagnetic field gradients is present in this second subregion 25 duringimage recording. Even after adjustment of all system components to theobject under examination, called shimming, a first subregion 26 a and 26b is present in which the magnetic field homogeneity and the gradientlinearity are lower than in the second subregion. The first subregioncan be defined by the fact that the relationship between the physicallocation in the MR system and the Larmor frequency of the spins deviatesby 5%, 7% or 10% in each case from the nominal value which is a linearrelationship between location and Larmor frequency when switching ofgradients is taking place and is a constant value when gradients areswitched off. Due to the increased inhomogeneity in the subregion 26 ato 26 b, here in the subregion of 26 b, there is an increased placementof tissue in a single pixel for the object under examination 24. Thephase encoding direction as shown in FIG. 2 is perpendicular to thedivision of the recording volume into the subregions. Artifacts 27having a high signal intensity can result which are caused by the factthat a plurality of pixels are placed on a single point, in other wordsa single pixel in the MR image, during the reconstruction. As a resultof incorrect calibration of the parallel imaging on account of the highsignal intensity, said artifacts 27 can at least partially fold overinto the field of view 25 as an additional artifact 27 b and overlay theobject 23 there, which can render the diagnosis more difficult. Suchartifacts 27 b can be reduced or prevented if the weighting matrix ofthe parallel imaging is calculated as explained in the following.

A detailed explanation is given in the following as to how a separatelyrecorded reference data set with a low resolution, and the use of amultispin echo sequence for creating the reference data set, can providedata that can be used to calculate a good kernel or a good weightingmatrix, which is then used in order to calculate missing raw data pointsduring the parallel imaging. The MR images then created have fewerartifacts due to the improved reference data set.

The imaging sequence for the creation of the actual MR image data can bea turbo spin echo Dixon imaging sequence. With this Dixon technique, thetissue components recorded in the object under examination have the samephase position once and the opposite phase position once. The MR imagesare recorded in a number of segments, which means that only a part ofthe raw data space is recorded (filled) per segment. Furthermore, theimaging sequence for creating the actual MR images is a multi-slicesequence. For each slice of the multi-slice sequence, the imagingsequence shown in FIG. 3 can be used in order to generate the referencedata set.

The sequence has an RF excitation pulse 30 and a number of refocusingpulses 31, 32 and 33. In particular, the refocusing pulses 32 and 33 andall subsequent refocusing pulses can be chosen in such a manner thatvery small refocusing angles are used, for example between 20° and 120°,preferably between 20° and 80°, further preferably between 20° and 60°.Simultaneously with the excitation pulses, the slice selection gradients40, 40 a, 41 and 42 are switched in the slice selection direction, the Zdirection of FIG. 3, as they are usually used in spin echo sequences. Inthe phase encoding direction, the gradients 38 and 39 as well as othergradients having different strengths are used for phase encoding and thesignal echoes generated by the refocusing pulses are read out during thereadout gradients 34, 35-37. This is illustrated schematically by theADC 43, 44 and 45. The imaging sequence used to generate the referencedata set differs here from the imaging sequence which is used forcreating the imaging data set. Thus it is possible that the excitationpulse 30 and the refocusing pulses 31, 32 or 33 have the same bandwidth.This is usually not the case with the RF pulses of the imaging sequenceused to create the imaging data set. As a result of the higher bandwidthand the smaller flip angles, shorter durations can be used for theirradiation by the excitation and refocusing pulses. Thus for example,the average duration which is used for the excitation pulses andrefocusing pulses is shorter by a factor of 0.6, 0.7 or 0.8 than thecorresponding average duration which occurs with the excitation pulsesand refocusing pulses of the imaging sequence for creating the imagingdata set. In addition, the resolution in the readout direction is lowerby a factor of 4 to 10 than during the creation of the imaging data set.Furthermore, different slice profiles can be used for the RF excitationpulses and refocusing pulses than for the associated RF excitationpulses and refocusing pulses used for creating the imaging data set. Aprecisely rectangular slice profile is not required for the referencedata set, which in turn means that the recording time overall can beshortened by using other slice profiles which place less emphasis on arectangular slice profile. The sensitivity of the reference data set toaliasing artifacts from the marginal region of the FOV is reduced by theabove-mentioned measures.

Preferably, the slice position for the generation of the MR images andthus of the reference data set is located in the coronary or sagittaldirection, where inhomogeneities occur at the edges due to the geometryof the MR system. The invention, however, can also be used fortransverse slice positioning.

By using the reference data set described above, said reference data setcan be recorded in total in a very short period of time, which meansthat the total time for recording the imaging data set is likewisereduced. The reference data generated by the reference data imagingsequence of FIG. 3 have a high degree of homogeneity in the image dataspace. This makes it possible to calculate the weighting kernel moreaccurately with this reference data set than with a reference data setintegrated in the imaging set, which is used in order to subsequentlyreconstruct the unrecorded raw data points in parallel imaging, recordedwith the aid of GRAPPA or SENSE techniques. How the weighting matrix iscalculated from the reference data set is known to those skilled in theart and thus need not be explained in detail herein. The RF pulses usedin the creation of the reference data set furthermore have the advantagethat they result in very low RF loads on the person under examination.

FIG. 4 summarizes the steps which enable missing raw data points to becalculated in parallel imaging, wherein the reference data set isrecorded as explained in FIG. 3 in order to create a homogeneousreference data set which forms a good basis for calculating theweighting matrix for determining the missing raw data points. The methodstarts in a step S51 and the reference data set is recorded in a stepS52, as explained above in connection with FIG. 3. In this case, thereference data set is recorded for each imaging slice of an imaging dataset. The recording of the individual slices is preferably carried outsuch that the data for a first slice are first recorded in theirentirety. Subsequently, the data of a second slice are recorded in theirentirety. The second slice can be directly adjacent to the first sliceor can be located at a different position in the slice package, forexample in the third position. When all the slices of the slice packagehave been recorded, the weighting matrix can subsequently be calculatedfor each slice, which then forms the basis for calculating the missingraw data points (step 52). The imaging data set is then recorded in astep S53. The recording of the imaging data set takes place in segmentedfashion as a general rule. In this regard a first set of k-space linesis first recorded from a first slice, for example every eighth k-spaceline of the raw data matrix. Subsequently, every eighth k-space line ofa second slice is recorded, etc. When this first number of k-space lineshas been recorded for every slice, a second pass of the entire slicepackage takes place after the repetition time TR. Here, a second set ofk-space lines of the raw data matrix is recorded for each slice. Theprocess is repeated until all necessary k-space lines have beenrecorded. The missing raw data points are then determined in step S54with the use of the weighting matrix and with the use of the raw datapoints recorded in step S53. Furthermore, in step S55 the MR images ofthe imaging data set are reconstructed. The reconstructed MR images havefewer artifacts and overall the recording time is reduced because therecording time for the creation of the reference data set can bereduced.

Although modifications and changes may be suggested by those skilled inthe art, it is the intention of the Applicant to embody within thepatent warranted hereon all changes and modifications as reasonably andproperly come within the scope of the Applicant's contribution to theart.

1. A method for operating a magnetic resonance (MR) apparatus, having anMR data acquisition scanner, in order to acquire MR data from anexamination subject with parallel imaging, said method comprising: froma computer, emitting reference data acquisition control signals to theMR data acquisition scanner in order to operate the MR data acquisitionscanner so as to acquire reference data from the examination subject,and entering the reference data into a memory organized as k-space forsaid reference data, with at least one sub-section of k-space for saidreference data being completely filled with said reference dataaccording to the Nyquist condition; from said computer, emitting MR rawdata acquisition control signals to said MR data acquisition scanner inorder to operate the MR data acquisition scanner to execute a parallelimaging spin-echo sequence in which MR raw data are acquired during spinechoes, and entering the acquired MR raw data into a memory organized ask-space for said MR raw data, with said MR raw data not completelyfilling k-space for said raw data according to the Nyquist condition,said MR raw data entered into k-space forming a raw data set; in saidcomputer, calculating a weighting matrix from said reference data set,and using said weighting matrix to calculate raw data, for raw datapoints in k-space for said raw data that were not filled with raw dataduring said parallel imaging, thereby obtaining a completed raw dataset; from said computer, emitting said reference data acquisitioncontrol signals and said MR raw data acquisition control signals to saidMR data acquisition scanner so as to acquire said MR raw data with saidspin-echo sequence without segmentation within an imaging slice andwithout temporal overlap with acquisition of said MR raw data set, andwith a resolution of said reference data in a readout direction that islower by at least a factor of 4 than a resolution of said MR raw data;and making the completed MR raw data set available from said computer inelectronic form as a data file.
 2. A method as claimed in claim 1comprising emitting said MR raw data acquisition control signals to saidMR data acquisition scanner in order to operate said MR data acquisitionscanner so as to acquire said MR raw data in a segmented recordingprocedure in a plurality of imaging slices of the examination subject,and emitting said reference data acquisition control signals so as tooperate said MR data acquisition scanner to acquire said reference datafor each of said plurality of imaging slices.
 3. A method as claimed inclaim 1 comprising emitting said MR raw data acquisition control signalsin order to operate said MR data acquisition scanner so as to radiate anRF excitation pulse, having a slice profile, in order to generate saidspin echoes, and emitting said reference data acquisition controlsignals so as to operate the MR data acquisition scanner in order toradiate an RF excitation pulse for acquiring said reference data, saidRF excitation pulse for acquiring said reference data having a differentslice profile from said RF excitation pulse that generates said spinechoes.
 4. A method as claimed in claim 1 comprising emitting said MRraw data acquisition control signals in order to operate said MR dataacquisition scanner so as to radiate an RF refocusing pulse, having aslice profile, in order to generate said spin echoes, and emitting saidreference data acquisition control signals so as to operate the MR dataacquisition scanner in order to radiate an RF refocusing pulse foracquiring said reference data, said RF refocusing pulse for acquiringsaid reference data having a different slice profile from said RFrefocusing pulse that generates said spin echoes.
 5. A method as claimedin claim 1 comprising emitting said MR raw data acquisition controlsignals in order to operate the MR data acquisition scanner so as toradiate a plurality of RF refocusing pulses, each having a flip angle,starting with a first RF refocusing pulse, to generate said spin echoes,and emitting said reference data acquisition control signals in order tooperate the MR data acquisition scanner so as to radiate a plurality ofRF refocusing pulses, starting with a first RF refocusing pulse, toacquire said reference data, with the RF refocusing pulses after saidfirst RF refocusing pulse for acquiring said reference data having asmaller flip angle than the RF refocusing pulses after the first RFrefocusing pulse for acquiring said MR raw data.
 6. A method as claimedin claim 5 comprising emitting said reference data acquisition controlsignals in order to operate the MR data acquisition scanner so as toradiate said RF refocusing pulses after said first RF refocusing pulsefor acquiring said reference data set with respective flip angles in arange between 20° and 120°.
 7. A method as claimed in claim 5 comprisingemitting said reference data acquisition control signals in order tooperate the MR data acquisition scanner so as to radiate said RFrefocusing pulses after said first RF refocusing pulse for acquiringsaid reference data set with respective flip angles in a range between20° and 70°.
 8. A method as claimed in claim 1 comprising emitting saidMR raw data acquisition control signals in order to operate said MR dataacquisition scanner so as to radiate RF excitation pulses and RFrefocusing pulses, each having a spectral bandwidth, in said spin-echosequence, and emitting said reference data acquisition control signalsin order to operate the MR data acquisition scanner so as to radiate RFexcitation pulses and RF refocusing pulses to acquire said referencedata, which have a spectral bandwidth that is independent of thespectral bandwidth of the RF excitation pulses and the RF refocusingpulses in said spin-echo sequence.
 9. A method as claimed in claim 8comprising emitting said reference data acquisition control signals inorder to operate the MR data acquisition scanner to radiate said RFexcitation pulses and said RF refocusing pulses for acquiring saidreference data with a same spectral bandwidth.
 10. A method as claimedin claim 1 comprising emitting said MR raw data acquisition controlsignals in order to operate said MR data acquisition scanner so as toradiate RF pulses, having an average duration, in said spin-echosequence, and emitting said reference data acquisition control signalsin order to operate the MR data acquisition scanner to radiate RF pulsesfor acquiring said reference data that have an average duration that isshorter by a factor of at least 0.8 than the average duration of the RFpulses in said spin-echo sequence.
 11. A method as claimed in claim 1comprising emitting said MR raw data acquisition control signals inorder to operate said MR data acquisition scanner so as to radiate RFpulses, having an average duration, in said spin-echo sequence, andemitting said reference data acquisition control signals in order tooperate the MR data acquisition scanner to radiate RF pulses foracquiring said reference data that have an average duration that isshorter by a factor of at least 0.6 than the average duration of the RFpulses in said spin-echo sequence.
 12. A method as claimed in claim 1comprising emitting said MR raw data acquisition control signals inorder to operate said MR data acquisition scanner to execute saidspin-echo sequence as a turbo spin-echo Dixon sequence in which spinechoes of different tissue components of said examination subject have asame phase position at least once, and an opposite phase position atleast once.
 13. A magnetic resonance (MR) apparatus comprising: an MRdata acquisition scanner; a computer configured to emit reference dataacquisition control signals to the MR data acquisition scanner in orderto operate the MR data acquisition scanner so as to acquire referencedata from the examination subject, and entering the reference data intoa memory organized as k-space for said reference data, with at least onesub-section of k-space for said reference data being completely filledwith said reference data according to the Nyquist condition; saidcomputer being configured to emit MR raw data acquisition controlsignals to said MR data acquisition scanner in order to operate the MRdata acquisition scanner to execute a parallel imaging spin-echosequence in which MR raw data are acquired during spin echoes, andentering the acquired MR raw data into a memory organized as k-space forsaid MR raw data, with said MR raw data not completely filling k-spacefor said raw data according to the Nyquist condition, said MR raw dataentered into k-space forming a raw data set; said computer beingconfigured to calculate a weighting matrix from said reference data set,and using said weighting matrix to calculate raw data, for raw datapoints in k-space for said raw data that were not filled with raw dataduring said parallel imaging, thereby obtaining a completed raw dataset; said computer being configured to emit said reference dataacquisition control signals and said MR raw data acquisition controlsignals to said MR data acquisition scanner so as to acquire said MR rawdata with said spin-echo sequence without segmentation within an imagingslice and without temporal overlap with acquisition of said MR raw dataset, and with a resolution of said reference data in a readout directionthat is lower by at least a factor of 4 than a resolution of said MR rawdata; and said computer being configured to make the completed MR rawdata set available from said computer in electronic form as a data file.14. A non-transitory, computer-readable data storage medium encoded withprogramming instructions, said storage medium being loaded into acomputer of a magnetic resonance (MR) apparatus comprising an MR dataacquisition scanner, said programming instructions causing said computerto: emit reference data acquisition control signals to the MR dataacquisition scanner in order to operate the MR data acquisition scannerso as to acquire reference data from the examination subject, andentering the reference data into a memory organized as k-space for saidreference data, with at least one sub-section of k-space for saidreference data being completely filled with said reference dataaccording to the Nyquist condition; emit MR raw data acquisition controlsignals to said MR data acquisition scanner in order to operate the MRdata acquisition scanner to execute a parallel imaging spin-echosequence in which MR raw data are acquired during spin echoes, andentering the acquired MR raw data into a memory organized as k-space forsaid MR raw data, with said MR raw data not completely filling k-spacefor said raw data according to the Nyquist condition, said MR raw dataentered into k-space forming a raw data set; calculate a weightingmatrix from said reference data set, and using said weighting matrix tocalculate raw data, for raw data points in k-space for said raw datathat were not filled with raw data during said parallel imaging, therebyobtaining a completed raw data set; emit said reference data acquisitioncontrol signals and said MR raw data acquisition control signals to saidMR data acquisition scanner so as to acquire said MR raw data with saidspin-echo sequence without segmentation within an imaging slice andwithout temporal overlap with acquisition of said MR raw data set, andwith a resolution of said reference data in a readout direction that islower by at least a factor of 4 than a resolution of said MR raw data;and make the completed MR raw data set available from said computer inelectronic form as a data file.